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Figure 2is the relationship between the heat conduction coefficient and the thickness of air.
Design of VIC involves trade-offs between the heat conduction through the multi-layer structure and the mechanical strength.
Therefore, the cross coupling between the heat conduction in the fluid and particle manifests itself as thermal waves at the macroscale.
With the coupling between the heat conduction in the fluid and particle phases denoted by β and σ- phases, respectively, the temperature T obeys the following energy equations [1, 2] γ β ∂ T β ∂ t = k β β Δ T β + k β σ Δ T σ + h a υ ( T σ − T β ) (8). and γ σ ∂ T σ ∂ t = k σ σ Δ T σ + k σ β Δ T β − h a υ ( T σ − T β ) (9).
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The decomposition algorithm uses a composite cylindrical surface source solution to deal with the composite heat conduction along the radius and a coil line source solution to deal with the heat conduction between tube loops in depth direction.
This article deals with the heat conduction across the interface between a thin isotropic thermal barrier coating and an anisotropic substrate by the boundary element method.
The heat conduction through the gas layer between sphere and plate is identified as the dominating mechanism.
First, there is the heat conduction in the two semiconductor legs between the source and the sink.
By constructing a special technique, the changes of heat conduction of air were studied by means of measuring the heat conduction with heat conduction instrument in NS between the hot plate and the cooling plate.
While the actual distance between vital pulp and occlusal surface is a decisive factor for the heat conduction into the tooth, this distance is unfortunately very variable and unpredictable [ 10].
Eq. 11 shows the heat conduction coefficient.
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